• Aucun résultat trouvé

Mathematical Analysis/Partial Differential Equations

N/A
N/A
Protected

Academic year: 2023

Partager "Mathematical Analysis/Partial Differential Equations"

Copied!
6
0
0

Texte intégral

(1)

http://france.elsevier.com/direct/CRASS1/

Mathematical Analysis/Partial Differential Equations

Lifting default for S 1 -valued maps

Petru Mironescu

Université de Lyon, Université Lyon1, CNRS, UMR 5208, institut Camille-Jordan, bâtiment du Doyen Jean-Braconnier, 43, boulevard du 11 novembre 1918, 69200 Villeurbanne cedex, France

Received and accepted 30 July 2008 Available online 23 August 2008

Presented by Haïm Brezis

Abstract

LetϕC([0,1]N,R). When 0< s <1,p1 and 1sp < N, theWs,p-semi-norm|ϕ|Ws,p ofϕis not controlled by

|g|Ws,p, whereg:=eıϕ[J. Bourgain, H. Brezis, P. Mironescu, Lifting in Sobolev spaces, J. Anal. Math. 80 (2000) 37–86]. [This question is related to existence, forS1-valued mapsg, of a liftingϕ as smooth as allowed byg.] In [J. Bourgain, H. Brezis, P. Mironescu, Lifting, degree, and distributional Jacobian revisited, Commun. Pure Appl. Math. 58 (2005) 529–551], the authors suggested that|g|Ws,pdoes control a weaker quantity, namely|ϕ|Ws,p+W1,sp. Existence of such control is due to J. Bourgain and H. Brezis [J. Bourgain, H. Brezis, On the equation divY =f and application to control of phases, J. Amer. Math. Soc. 16 (2003) 393–426] when 1< p2,s=1/pand to H.-M. Nguyen [H.-M. Nguyen, Inequalities related to liftings and applications, C. R.

Acad. Sci. Paris, Ser. I 346 (17–18) (2008) 957–962] whenN=1,p >1 andsp1 or whenN2,p >1 andsp >1. In this Note, we establish existence of control for alls <1,p1 andN.To cite this article: P. Mironescu, C. R. Acad. Sci. Paris, Ser. I 346 (2008).

©2008 Académie des sciences. Published by Elsevier Masson SAS. All rights reserved.

Résumé

Défaut de relèvement pour les applications à valeurs dans le cercle unité.SoitϕC([0,1]N,R). Si 0< s <1,p1 et 1sp < N, alors la semi-norme|ϕ|Ws,p n’est pas contrôlée par|g|Ws,p, oùg:=eıϕ[J. Bourgain, H. Brezis, P. Mironescu, Lifting in Sobolev spaces, J. Anal. Math. 80 (2000) 37–86]. [Cette question est liée à l’existence, pour desgà valeurs dansS1, de relèvementsϕaussi réguliers quegle permet.] Dans [J. Bourgain, H. Brezis, P. Mironescu, Lifting, degree, and distributional Jacobian revisited, Commun. Pure Appl. Math. 58 (2005) 529–551], il est conjecturé que|g|Ws,pcontrôle une quantité plus faible que|ϕ|Ws,p, plus spécifiquement|ϕ|Ws,p+W1,sp. L’existence d’un tel contrôle est due à J. Bourgain and H. Brezis [J. Bourgain, H. Brezis, On the equation divY=f and application to control of phases, J. Amer. Math. Soc. 16 (2003) 393–426] pour 1< p2 ets=1/pet à H.-M. Nguyen [H.-M. Nguyen, Inequalities related to liftings and applications, C. R. Acad. Sci. Paris, Ser. I 346 (17–18) (2008) 957–962] pourN=1,p >1 etsp1 ou pourN2,p >1 etsp >1. Dans cette Note, nous montrons l’existence d’un contrôle pour touts <1,p1 etN.Pour citer cet article : P. Mironescu, C. R. Acad. Sci. Paris, Ser. I 346 (2008).

©2008 Académie des sciences. Published by Elsevier Masson SAS. All rights reserved.

E-mail address:[email protected].

1631-073X/$ – see front matter ©2008 Académie des sciences. Published by Elsevier Masson SAS. All rights reserved.

doi:10.1016/j.crma.2008.08.001

(2)

Version française abrégée

SoientC= [0,1]N, 0< s <∞et 1p <∞.| |Ws,p désigne une semi-norme standard sur l’espace de Sobolev Ws,p(C); par exemple, pour 0< s <1 nous considérons la semi-norme de Gagliardo,

|u|Ws,p =

C2

|u(x)u(y)|p

|xy|N+sp dxdy 1/p

.

Si ϕC(C,R)etg:=eıϕ, alors |∇ϕ| = |∇g|. En particulier,|g|W1,p = |ϕ|W1,p. Plus généralement, |g|Ws,p

contrôle|ϕ|Ws,p sis1, au sens où il existe une inégalité de la forme|ϕ|Ws,p F (|g|Ws,p)avecF croissante [3].

Ceci n’est plus forcément vrai si 0< s <1. Voici un exemple inspiré de [3] : siN 2 et si 0< s <1 etp sont tels que 1< sp < N, alors il existe une fonction ψW1,sp\Ws,p. Si on considère ϕε:=ψρε, avecρ noyau régularisant, alors|ϕε|Ws,p → ∞(carψ /Ws,p), alors quegε:=eıϕε reste bornée dansW1,spL(carψW1,sp) et donc dans Ws,p, grâce à l’inclusion de Gagliardo–NirenbergW1,spLWs,p. Nonobstant la non inclusion W1,1LWs,psisp=1, on peut adapter cet exemple au cas oùsp=1 etN1. Plus généralement, sisp=1 ou 1< sp < N, alors on peut obtenir l’absence du contrôle à partir d’une fonction convenableψWs,p+W1,sp.

Dans le cas particuliers=1/2 etp=2, J. Bourgain et H. Brezis [2] ont montré que le contre-exemple ci-dessus est essentiellement le seul. Leur résultat est que toute fonctionϕ se décompose commeϕ=ϕ1+ϕ2, où|ϕ1|H1/2 et

|ϕ2|W1,1sont contrôlées par|g|H1/2. La preuve s’étend aux espacesW1/p,pavec 1< p2 et donne la décomposition (1). Ce résultat a motivé le problème suivant [4,8] avec 0< s <1 et 1p <∞:

(Ds,p) ToutϕC(C,R)s’écritϕ=ϕ1+ϕ2, où|ϕ1|Ws,pC|eıϕ|Ws,p et2LspC|eıϕ|1/sWs,p.

Récemment, H.-M. Nguyen [10] a résolu ce problème lorsque p >1, s=1/petN =1 ; son argument s’applique aussi au casN2,p >1 etsp >1.

Le but de cette Note est d’annoncer le suivant :

Théorème 1.La décomposition(Ds,p)est valide pour tout0< s <1,p1etN.

Notons que la décomposition existe même sisp <1.

Idée de la preuve. On étendgà une applicationh:RN→R2, de sorte quehsoit Lipschitz, constante en dehors d’un compact,|h|3 et|h|Ws,p(RN)C|g|Ws,p(C). On étend ensuitehàRN×R+par la formulew(x, ε)=Π (hρε(x)).

Ici,ΠC(R2;R2)est telle queΠ (z)=z/|z|si|z|1/2, tandis queρC0satisfaitρ0,

ρ=1, suppρB(0,2)\B(0,1). Alors la conclusion du théorème est vérifiée parϕj données par

ϕ1(x):= −

0

w(x, ε)∂w

∂ε(x, ε)dε, ϕ2:=ϕϕ1.

L’inégalité|ϕ1|Ws,pC|h|Ws,p découle d’estimations standard1pour les régulariséeshρεd’une fonctionhWs,p. Elle implique|ϕ1|Ws,pC|g|Ws,p.

Pour estimer2, le point de départ est l’identité2

2(x)= −2

0

∂εw(x, ε)Dxw(x, ε)dε.

En adaptant une idée de [4], cette identité permet d’obtenir l’estimation2LspC|eıϕ|1/sWs,p. 2

1 L’une des estimations utilisées dans la preuve est RN

0 εpsp1|D[hρε](x)|pdxC|h|pWs,p, bien connue par les spécialistes [11], II.12.

2 Évidente, du moins formellement.

(3)

Le lecteur trouvera les preuves détaillées dans [9] ; entre autres, on y explique pourquoi notre décomposition est une sorte d’analogue continu de la décomposition trouvée dans [2].

1. Introduction

LetC= [0,1]N, 0< s <∞and 1p <∞. We will denote by| |Ws,p a standard semi-norm on the Sobolev space Ws,p(C); e.g., when 0< s <1, we take the Gagliardo semi-norm

|u|Ws,p=

C2

|u(x)u(y)|p

|xy|N+sp dxdy 1/p

.

LetϕC(C,R)and setg=eıϕ. Since|∇ϕ| = |∇g|, we have|g|W1,p= |ϕ|W1,p. More generally,|g|Ws,pcontrols

|ϕ|Ws,p when s1, i.e., there is some nondecreasing F such that |ϕ|Ws,p F (|g|Ws,p)[3]. This need not hold when 0< s <1. Here is an example, essentially taken from [3]: letN2 and let 0< s <1, 1p <∞be such that 1< sp < N. By a Sobolev “nonembedding”, there is someψW1,sp\Ws,p. Letϕε:=ψρε and setgε= eıϕε, whereρ is a mollifier. Then|ϕε|Ws,p → ∞(since ψ /Ws,p). On the other hand, gε:=eıϕε is bounded in W1,spL (sinceψW1,sp) and thus in Ws,p, by the Gagliardo–Nirenberg embeddingW1,spLWs,p. Despite the nonembeddingW1,1LWs,pwhensp=1, one may easily adapt this example to the casesp=1 andN1. More generally, whensp=1 or 1< sp < N, one may prove lack of control with the help of an appropriate ψWs,p+W1,sp.

In the special cases=1/2 andp=2, J. Bourgain and H. Brezis [2] proved that the above counter-example is essentially the only one. Their results asserts that each ϕ splits as ϕ=ϕ1+ϕ2, where |ϕ1|H1/2 and|ϕ2|W1,1 are controlled by|g|H1/2. Their argument adapts steadily to the spacesW1/p,pwhere 1< p2 and yields

If 1< p2, thenϕ=ϕ1+ϕ2

whereϕjC(C), |ϕ1|W1/p,pC|g|W1/p,p, |ϕ2|W1,1C|g|pW1/p,p. (1) This motivated the following open problem [4,8]:

(Ds,p) EachϕC(C,R)splits asϕ=ϕ1+ϕ2, where|ϕ1|Ws,p C|eıϕ|Ws,p and2LspC|eıϕ|1/sWs,p. [Here, 0< s <1 and 1p <∞.] Very recently, H.-M. Nguyen [10] answered positively this problem whenp >1, s=1/pandN=1; his argument adapts to the case whereN2,p >1 andsp >1.

The main purpose of this Note is to announce the following:

Theorem 1.The decomposition(Ds,p)holds for each0< s <1,p1andN. Unlike the proofs in [2,10], our method applies to the casesp <1.

2. Heuristics of the proof of Theorem 1

In order to explain the main idea, we consider, for simplicity, maps defined onRN which are constant at infin- ity (rather than maps defined on [0,1]N). Assume first thatϕ has small amplitude oscillations, say|ϕ| 1. Then

|g−1| 1 and|ϕ|Ws,p ∼ |g|Ws,p. Thus, in this case, a convenient decomposition isϕ1=ϕ andϕ2=0. We next proceed as follows: we derive a formula forϕ. This formula givesϕ only whenϕ has small amplitude oscillations, but we may give it a meaning for eachϕ. In general (i.e., whenϕmay oscillate), we take this formula as the definition ofϕ1and simply letϕ2be the phase excess, i.e., we setϕ2=ϕϕ1.

In order to obtain a tractable formula forϕ, we rely on the following remark: ifg=eıϕ, then there is no formula givingϕ in terms ofg, but there is one for Dϕ, since =gDg. We consider a smooth extension w:RN× [0,+∞[ →S1ofgsuch that

εlim→∞w(., ε)=const. (2)

(4)

A natural choice is w(x, ε)=Π (gρε(x)), whereΠ (z)=z/|z| andρ is a mollifier. This yields a smooth map wheneverg(and thusgρε) is close to 1. We may writew=eıψ, whereψ (x,0)=ϕ(x). Assuming that convergence in (2) is sufficiently fast, we than haveψ (x,)=Cand thus

ϕ(x)= −ψ (x, ε)|εε=∞=0 +C=C

0

w(x, ε)∂w

∂ε(x, ε)dε. (3)

As explained in the next section, (3) gives the right definition ofϕ1, provided we pick an appropriateρand we change slightly the definition ofΠ.

3. Sketch of the proof of Theorem 1

Let ϕC(C,R)and set g=eıϕ. We first extend gto a Lipschitz map h:RN →R2 such thath is constant outside[−1,2]N,|h|3 and|h|Ws,p(RN)C|g|Ws,p(C). We next extendhtoRN×R+through the formulaw(x, ε)= Π (hρε(x)). Here,ΠC(R2;R2)is such thatΠ (z)=z/|z|if|z|1/2, whileρC0satisfiesρ0,

ρ=1, suppρB(0,2)\B(0,1). Then the conclusion of the theorem holds withϕj given by

ϕ1(x):= −

0

w(x, ε)∂w

∂ε(x, ε)dε, ϕ2:=ϕϕ1. (4)

The inequality

|ϕ1|Ws,pC|h|Ws,p (5)

follows from standard estimates1for regularizationshρε of mapshWs,p. As a consequence of (5), we find that

|ϕ1|Ws,pC|g|Ws,p.

[Estimate (5) is a cousin of the estimate

x

0

uρε(x)∂

∂ε

vρε(x)

Ws,p

CuL|v|Ws,p, (6)

valid for any reasonable ρ and presumably well known to experts. For specialρ’s, the “discrete” and much more popular analog of (6) is the “paraproduct inequality” [7]

jk

ujvk Ws,p

CuL|v|Ws,p, (7)

whereu=

uj,v=

jvj are the Littlewood–Paley decompositions ofuandv. Both (6) and (7) are refinements of the standard inequalityuvWs,pC(uWs,pvL+ vWs,puL).]

The starting point for estimating2is the identity

2(x)= −2

0

∂εw(x, ε)Dxw(x, ε)dε. (8)

At least formally, this identity follows from

2(x)=Dϕ(x)+

0

Dxw(x, ε)

∂εw(x, ε)dε+

0

w(x, ε)

∂εDxw(x, ε)

1 One of the key estimates used in the proof is RN

0 εp−sp−1|D[hρε](x)|pdxC|h|pWs,p, well known to experts [11], II.12.

(5)

=w(x, ε)Dxw(x, ε)|ε=0+

0

Dxw(x, ε)

∂εw(x, ε)dε+w(x, ε)Dxw(x, ε)|εε=∞=0

0

∂εw(x, ε)Dxw(x, ε)dε= −2

0

∂εw(x, ε)Dxw(x, ε)dε.

Adapting an idea from [4], this identity implies the estimate2LspC|eıϕ|1/sWs,p. 2 The interested reader will find the detailed proof in [9].

We end this section by comparing our decomposition to the Bourgain–Brezis one. Assuming, for the sake of the simplicity, thatϕandgare defined on the wholeRN, the decomposition in [2] is (withg=

gjthe Littlewood–Paley decomposition ofg)

ϕ1:=

jk

gjgk, ϕ2:=ϕϕ1. (9)

In the same way (6) is related to (7), one may interpret the formula definingϕ1in (9) as a discrete analog of

x→ −

0

gρε(x)

∂ε

gρε(x) dε.

Thus our decomposition is a continuous version of the one in [2], with the additional sophistication that the regular- izations ofgare “almost projected” ontoS1(viaΠ).

4. Some applications

As a first application, we may achieve the description ofXs,p=C(C;S1)Ws,p, partly obtained in [3] and [5].

Theorem 2.Let0< s <,1p <. Then

(a) ([3]) Whensp <1orspN,Xs,p=Ws,p(C;S1);

(b) ([5]) Whens1andsp2,Xs,p=Ws,p(C;S1);

(c) ([5]) Whens1and1sp <2,Xs,p= {eıϕ;ϕWs,pW1,sp(C,R)};

(d) When0< s <1and1< sp < N,Xs,p= {eıϕ;ϕ(Ws,p+W1,sp)(C,R)};

(e) When0< s <1,N2andsp=1,Xs,p= {eıϕ;ϕ(Ws,p+W1,1)(C,R)} ∩Ws,p(C;S1).

The lack of symmetry between statements (d) and (e) is explained by the fact that, whensp >1 ands <1, we have ϕW1,speıϕWs,p; this implication fails whensp=1 ands <1. For the proof of (d) and (e), we send the reader to [9].

In a forthcoming joint paper with H. Brezis and H.-M. Nguyen [6], we investigate several consequences of Theo- rem 1. We end this Note by mentioning one of them.

Theorem 3.(See [6].) Assume thatN3,0< s <1,2sp < N,k∈ {2,3, . . .}. Then, for eachuWs,p(C;S1), there is somevWs,p(C;S1)such thatu=vk.

This answers a question of F. Bethuel and D. Chiron [1]. [For the other values ofs,pandN, the surjectivity of the mapvvkis clarified in [1]. The case considered in Theorem 3 is the only one left open in [1].]

Acknowledgements

The author thanks H.-M. Nguyen for sending him an early version of [10]. He warmly thanks P. Bousquet, H. Brezis and H.-M. Nguyen for useful discussions.

(6)

References

[1] F. Bethuel, D. Chiron, Some questions related to the lifting problem in Sobolev spaces, in: H. Berestycki, M. Bertsch, F. Browder, L. Nirenberg (Eds.), Perspectives in Nonlinear Partial Differential Equations, in: Contemporary Mathematics, vol. 446, Amer. Math. Soc., 2007, pp. 125–

152.

[2] J. Bourgain, H. Brezis, On the equation divY=f and application to control of phases, J. Amer. Math. Soc. 16 (2003) 393–426.

[3] J. Bourgain, H. Brezis, P. Mironescu, Lifting in Sobolev spaces, J. Anal. Math. 80 (2000) 37–86.

[4] J. Bourgain, H. Brezis, P. Mironescu, Lifting, degree, and distributional Jacobian revisited, Commun. Pure Appl. Math. 58 (2005) 529–551.

[5] H. Brezis, P. Mironescu, On some questions of topology forS1-valued fractional Sobolev spaces, Rev. R. Acad. Cien., Serie A Mat. 95 (2001) 121–143.

[6] H. Brezis, P. Mironescu, H.-M. Nguyen, in preparation.

[7] J.-Y. Chemin, Fluides parfaits incompressibles, Astérisque 230 (1995).

[8] P. Mironescu, Sobolev maps on manifolds: degree, approximation, lifting, in: H. Berestycki, M. Bertsch, F. Browder, L. Nirenberg, L.A.

Peletier, L. Véron (Eds.), Perspectives in Nonlinear Partial Differential Equations, In honor of Haïm Brezis, in: Contemporary Mathematics, vol. 446, Amer. Math. Society, 2007, pp. 413–436.

[9] P. Mironescu, Lifting ofS1-valued maps in sums of Sobolev spaces, J. European Math. Soc., submitted for publication.

[10] H.-M. Nguyen, Inequalities related to liftings and applications, C. R. Acad. Sci. Paris, Ser. I 346 (17–18) (2008) 957–962.

[11] H. Triebel, Theory of Function Spaces, Birkhäuser Verlag, 1983.

Références

Documents relatifs

Entropy methods in partial differential equations: fast diffusion equations –

Persson, Singular holomorphic solutions of linear partial differential equations with holomorphic coef- ficients and nonanalytic solutions of equations with analytic

First of all, Bonnet's theorem tells us that for a compact manifold with positive sectional curvature, the fundamental group must be finite and this was later generalized by

NIRENBERG Estimates near the boundary for solutions of elliptic partial differeratial equations satisfying general boundary conditions I. To appear

One of the important components of algebraic analysis is the study of analytic P-modules (i.e., modules over the ring of linear partial differential operators with

Theorem 1.1 has been used by Brezis, Marcus and Ponce [5] to study the existence of solutions of the nonlinear equation − u + g(u) = µ where µ is a measure and g is a

[r]

The principal local result, The Local Ex- tension Theorem (Appendix 6), is also the main step in all the appli- cations of the Convex Integration technique to solving open and